Defect and Diffusion Forum
Vol. 264
Vol. 264
Defect and Diffusion Forum
Vol. 263
Vol. 263
Defect and Diffusion Forum
Vols. 261-262
Vols. 261-262
Defect and Diffusion Forum
Vols. 258-260
Vols. 258-260
Defect and Diffusion Forum
Vols. 254-257
Vols. 254-257
Defect and Diffusion Forum
Vol. 253
Vol. 253
Defect and Diffusion Forum
Vols. 251-252
Vols. 251-252
Defect and Diffusion Forum
Vol. 250
Vol. 250
Defect and Diffusion Forum
Vol. 249
Vol. 249
Defect and Diffusion Forum
Vols. 247-248
Vols. 247-248
Defect and Diffusion Forum
Vols. 245-246
Vols. 245-246
Defect and Diffusion Forum
Vols. 242-244
Vols. 242-244
Defect and Diffusion Forum
Vol. 241
Vol. 241
Defect and Diffusion Forum Vols. 251-252
Paper Title Page
Abstract: The purpose of this work is to study the effect of bulk point defects on the electronic
structure of rutile TiO2. The paper is focused on the effect of oxygen nonstoichiometry in the form
of oxygen vacancies, Ti interstitials and Ti vacancies and related defect disorder on the band gap
width and on the local energy levels inside the band gap. Ab initio density functional theory is used
to calculate the formation energies of such intrinsic defects and to detect the positions of these
defect induced energy levels in order to visualize the tendency of forming local mid-gap bands.
Apart from the formation energy of the Ti vacancies (where experimental data do not exist) our
calculated results of the defect formation energies are in fair agreement with the experimental
results and the defect energy levels consistently support the experimental observations. The
calculated results indicate that the exact position of defect energy levels depends on the estimated
band gap and also the charge state of the point defects of TiO2.
1
Abstract: Three Zinc Molybdenum ceramic samples doped Bi have been prepared according to the
chemical formula (1-x) ZnO – 0.2MoO3 – xBi2O3, where (x = 0.2, 0.5, 1.0) mol %. The samples were
studied at room temperature through X-ray Diffraction analysis, SEM, EDAX, I-V characteristics and
C-V measurements. The results decleared the presences of two phases; ZnO as a major phase beside
Bi2MoO6 as a minor phase. At lower Bi additions; Bi and Mo ions are highly segregated at the grain
boundaries, while at higher additions more homogenous distribution for these ions inside the grain is
observed. Some pores are observed around the batches of the minor phase and at the grain
boundaries. The grain size is enlarged with increasing Bi addition; while the number and size of the
pores are decrease. Creation of the pores is attributed to oxygen liberation from the surface of the
sample during sintering. Formation of Schottky barrier is indicated via I-V and C-V measurements
and attributed to Zn vacancies at the grain boundary. Interface potential barrier, donor density,
interface state density and barrier width are decrease with increasing Bi addition. I-V characteristics
revealed voltage switching. The switching voltage E0 decreases with increasing Bi addition and it is
reproducible even after several on-off cycles.
13
Abstract: ZrW2O7(OH1-x,Clx)2·2H2O (x = 0.016, 0.025) is prepared by using the acid steam
hydrothermal (ASH) method. The chlorine contents of the crystals are measured by means of
potentiometric titration and ICP, respectively. The as-prepared powders are characterized by X-ray
diffraction, and their structures are refined by using the Rietveld method contained in the GSAS
program. The results indicate that the chloride ion occupies the hydroxyl group crystal site
statistically.
21
Abstract: We have investigated deep trap concentrations in hydride vapor pressure epitaxy (HVPE) - grown
GaN by measuring three-dimensional carrier concentration profiles and ionization energies.
Schottky contacts were fabricated on 28-68μm thick films using Ni/Au contacts. Extensive
capacitance-voltage measurements were made in the temperature range 100-350K at reverse bias
voltages in the range 0 to –5V. Effective carrier concentrations and ionization energies were
determined from three-dimensional plots of concentration-temperature-depth. Carrier concentration
versus temperature plots show slowly changing three-step behavior. During the first step, all the
plots rise linearly up to about 200K reaching respective plateaus before reversing courses
downwards again linearly. Ionization energy plots, on the other hand, are almost linear all the way
up to 350 K showing some tendency of upward bending. Trap concentrations were determined from
carrier concentrations and previously measured deep level transient spectroscopy (DLTS) plots as
function of reverse bias voltages. In almost every case, trap concentrations also rise linearly with
increasing depth in the samples.
35
Abstract: The mechanism of slow positron annihilation in Si-doped GaAs has been discussed in
terms of the diffusion trapping model (DTM). The trapping of positrons has been considered in
SiAs acceptors i.e. shallow defects and in VGa-SiGa vacancy complexes. The model has been used
to obtain the Doppler broadening line shape parameter (S-parameter) and average positron
lifetime in Si-doped GaAs, for a temperature range 20K to 290K and for different doping
concentrations. Observations are made regarding the effect of doping on the nature and
concentration of point defects. The change in point defect concentration due to Si- doping has
been found to be proportional to the doping concentration. The effect of detrapping from the
shallow defects has been found to be important at higher temperatures.
51
Abstract: The six-jump-cycle (6JC) mechanism is used to derive expressions for collective
correlation factors in a nonstoichiometric binary intermetallic compound AB. The 6JC is used as
a fundamental unit for the cycle involving a perfectly ordered configuration and a two-jumpcycle
(2JC) as a fundamental unit for the cycle involving existing antistructural atoms. The
jump frequency for the 6JC is calculated in terms of a four-frequency-model using the mean
first passage concept of Arita et al., while the jump frequency for the 2JC is taken to be the
harmonic mean of the individual jump frequencies. The expressions for phenomenological
transport coefficients are obtained through the linear response approximation using the kinetic
equation approach. The results for collective correlation factors are compared with Monte Carlo
simulation and are found to be in reasonably good agreement when the ratio of jump
frequencies of regular site and antistructural atoms is of the order of 10-1.
59
Abstract: The six-jump-cycle (6JC) diffusion mechanism is used to analyze the behavior of
vacancy-wind factors and collective correlation factors in partially ordered B2 intermetallic
compounds at stoichiometric and near- stoichiometric compositions. Expressions for the vacancywind
factors are obtained in the framework of the four-frequency model where the two sublattices
exist a priori. The phenomenological coefficients on the two sublattices that remain hitherto
independent in 6JC mechanism are connected through a microscopic detailed balance condition.
The present results for collective correlation factors when compared with our earlier calculation
based on taking the harmonic mean of the sublattice correlation factors show much better agreement
with Monte Carlo simulation results. The collective correlation factors and tracer correlation factors
are used to calculate the vacancy-wind factors. Our results for vacancy-wind factors agree
qualitatively with the simulation data when the frequency ratio ( α ) of structural and antistructural
atoms jumps decreases up to the order of unity.
69
Abstract: Positron Annihilation Doppler Broadening Spectroscopy (PADPS) is one of the nuclear
techniques used in material science. PADPS measurements are used to study the behavior of defect
concentration and dislocation density in a set of 3003 and 3005 wrought aluminum alloy. It has
been shown that positrons can become trapped at imperfect locations in solids. The S-parameter can
be influenced by changes in the concentration of such defects. There is no observed change in the Sparameter
values after the saturation of defect concentration. The S-parameter and trapping rates for
the samples deformed up to 10 percent were studied. The concentration of defect range varies from
1017 to 1018 cm-3 and from 1016 to 1017 cm-3 for 3003 and 3005 wrought Al alloy respectively. While
trapping rate range varies from 1 x1010 to 1.2x1011 s-1 for 3003 and from 1 x109 to 1.2x1010 s-1 for
3005 wrought Al alloy.
79
Abstract: Creep experiments were conducted on Cu-8.5at.% Al alloy in the intermediate temperature range
from 673 to 873K, corresponding to 0.46-0.72 Tm where Tm is the absolute melting temperature.
The present analysis reveals the presence of two distinct deformation regions (climb and viscous
glide) in the plot of log ε vs. log σ. The implications of these results on the transition from powerlaw
to exponential creep regime are examined. The results indicated that the rate controlling
mechanism for creep is the obstacle-controlled dislocation glide. A phenomenological model is
proposed which assumes that cell boundaries with sub-grains act as sources and obstacles to gliding
dislocations.
89